2016
DOI: 10.1119/1.4953167
|View full text |Cite
|
Sign up to set email alerts
|

Numerical solutions of reaction-diffusion equations: Application to neural and cardiac models

Abstract: We describe the implementation of the explicit Euler, Crank-Nicolson, and implicit alternating direction methods for solving partial differential equations and apply these methods to obtain numerical solutions of three excitable-media models used to study neurons and cardiomyocyte dynamics. We discuss the implementation, accuracy, speed, and stability of these numerical methods.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

0
3
0

Year Published

2019
2019
2024
2024

Publication Types

Select...
5
1
1

Relationship

0
7

Authors

Journals

citations
Cited by 8 publications
(3 citation statements)
references
References 42 publications
0
3
0
Order By: Relevance
“…5 ) with time step and spatial step . Such discretization satisfies the criterion of stability for the difference schemes , where D is the diffusion coefficient 16 , 53 . To implement no-flux boundary conditions for an arbitrary cell shape, we applied the modified five-point stencil of the 2D Laplace operator , so that: where is the concentration of , or in position at time , is the binary mask representing the cell ( ) and the background ( ), is the diffusion coefficient of or (while the diffusion of the component is negligible) and is the reaction term (see Eqs.…”
Section: Methodsmentioning
confidence: 99%
“…5 ) with time step and spatial step . Such discretization satisfies the criterion of stability for the difference schemes , where D is the diffusion coefficient 16 , 53 . To implement no-flux boundary conditions for an arbitrary cell shape, we applied the modified five-point stencil of the 2D Laplace operator , so that: where is the concentration of , or in position at time , is the binary mask representing the cell ( ) and the background ( ), is the diffusion coefficient of or (while the diffusion of the component is negligible) and is the reaction term (see Eqs.…”
Section: Methodsmentioning
confidence: 99%
“…(1) and (2) numerically using the forward time centered space method. 20,21 The fields are discretized on a 128 × 128 grid, such that x = j∆, y = i∆, t = nδt and i, j, n ∈ N. Differential operators are replaced by forward and central finite differences with spacing ∆ = 1 (length units) and time step δt = 0.25 (time units), as illustrated in Fig. 1(c).…”
Section: The Gray-scott Modelmentioning
confidence: 99%
“…Mainly, semi-linear reaction-diffusion PDEs are commonly used to model a variety of real-world phenomenon such as population dynamics and chemical reactions etc., [31], [40]. Many researchers have focused their attention on reactiondiffusion equations due to their wide range of applications, see [1], [11], [12], [17], [25], [33]. Random noise in dynamical systems is caused by external disruptions, measurement errors, and a lack of knowledge of specific parameters.…”
Section: Introductionmentioning
confidence: 99%